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Consider a causal LTI system implemented as the RL circuit shown below. In this circuit, v(t) is the input voltage. The curre

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Solution Güven circuit mm ults = input VCL) ilts = output to kvL in the ciruit from - -u(t) ti (1) R+ L dilts to dt voltage a3 H(S) - 10 - at Substitute s=jw Hljus 1(jw) - On vw) 1 JWLtra ut- tint =) W- 1 rad see R = lor, i=1 H = JXL = 1 WL=i1 R JXL ilus on .) a les ucts = 120 vt) DE ILO - ilm = - VCE) RtjXL IVw.)?7R² V 1²+ 102 10.oug 0.0995 - e 0.01 * BI LH (gw) 0= - tant Ecoo Wz cod = -tan (1) Os -5.710 3) i(t) = 1.0.01). Sin It-0I since there is no pole at origin before 10 gad/sec, the plot will be a straight line parallel to w-axis. - And then the ploat We 100 -200g 10010 -20dB doo wa 1000 - 2000g 1000= 10 -40dB Frode I w WKL Wc I LH (jw) s want - - tań (07-01 w = 10 > tan) magnita de plot of HjW) resembles the property of a high pass filter where frequencies below certain frequency Called Comer

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